MAC 2313 Lecture Notes - Lecture 3: Cross Product, Parallelogram, Euclidean Geometry

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In this lecture we again de ne a new product for vectors. In this case, the multiplication of two vectors yields a third vector with some very interesting properties and applications. The cross product of the vectors u and v, represented symbolically as u v, is de ned to be a vector of magnitude. |u v| = where (cid:18) is the angle (0 (cid:18) (cid:25)) between the vectors and where the resulting product vector has a direction given by the right hand rule. The rst results of the de nition of the cross products are given in the following theorem: The de nition of the cross product does not provide a con- venient means of computation for component-wise represen- tations of vectors. Let u = u1; u2; u3 and v = v1; v2; v3 , then u v = (cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12) (cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12)(cid:12) : j i k u1 u2 u3 v3 v1 v2.

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